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Measurement of the $^{16}$O(n, α)$^{13}$C cross-section using a Double Frisch Grid Ionization Chamber

The $^{16}$O(n, α)$^{13}$C reaction was proposed to be measured at the neutron time-of-flight (n_TOF) facility of CERN. To this purpose, a Double Frisch Grid Ionization Chamber (DFGIC) containing the oxygen atoms as a component in the counting gas coupled with a switch device in order to prevent the...

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Autores principales: Urlass, Sebastian, Beyer, Roland, Hammer, Sebastian, Hartmann, Andreas, Junghans, Arnd R, Kögler, Toni, Lutz, Benjamin, Mingrone, Federica, Müller, Stefan, Römer, Katja, Scheibler, Daniela, Stach, Daniel, Szücs, Tamás, Tassan, Laurent-Got, Turkat, Steffen, Wagner, Andreas, Weinberger, David
Lenguaje:eng
Publicado: 2020
Materias:
Acceso en línea:https://dx.doi.org/10.1051/epjconf/202023901030
http://cds.cern.ch/record/2800364
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author Urlass, Sebastian
Beyer, Roland
Hammer, Sebastian
Hartmann, Andreas
Junghans, Arnd R
Kögler, Toni
Lutz, Benjamin
Mingrone, Federica
Müller, Stefan
Römer, Katja
Scheibler, Daniela
Stach, Daniel
Szücs, Tamás
Tassan, Laurent-Got
Turkat, Steffen
Wagner, Andreas
Weinberger, David
author_facet Urlass, Sebastian
Beyer, Roland
Hammer, Sebastian
Hartmann, Andreas
Junghans, Arnd R
Kögler, Toni
Lutz, Benjamin
Mingrone, Federica
Müller, Stefan
Römer, Katja
Scheibler, Daniela
Stach, Daniel
Szücs, Tamás
Tassan, Laurent-Got
Turkat, Steffen
Wagner, Andreas
Weinberger, David
author_sort Urlass, Sebastian
collection CERN
description The $^{16}$O(n, α)$^{13}$C reaction was proposed to be measured at the neutron time-of-flight (n_TOF) facility of CERN. To this purpose, a Double Frisch Grid Ionization Chamber (DFGIC) containing the oxygen atoms as a component in the counting gas coupled with a switch device in order to prevent the charge collection from the so-called γ-flash has been developed at Helmholtz-Zentrum Dresden-Rossendorf (HZDR), in Germany. The first $^{16}$O(n, α)$^{13}$C measurement without seeing the charge of the γ-flash at n_TOF has been performed in November 2018. After the electronics did not suffer from the γ-flash any more, another huge charge collection was discovered. Due to the high instantaneous flux at the n_TOF facility [1] the amount of that induced charge from neutron induced background reactions was piling up so much that the recognition of $^{16}$O(n, α)$^{13}$C reactions from that background was very difficult. For that reason another $^{16}$O(n, α)$^{13}$C measurement at the time-of-flight facility nELBE at HZDR which has a low instantaneous flux [2], has been performed in April 2019. Both measurements from n_TOF and nELBE will be presented here.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2020
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spelling cern-28003642022-01-25T22:17:04Zdoi:10.1051/epjconf/202023901030http://cds.cern.ch/record/2800364engUrlass, SebastianBeyer, RolandHammer, SebastianHartmann, AndreasJunghans, Arnd RKögler, ToniLutz, BenjaminMingrone, FedericaMüller, StefanRömer, KatjaScheibler, DanielaStach, DanielSzücs, TamásTassan, Laurent-GotTurkat, SteffenWagner, AndreasWeinberger, DavidMeasurement of the $^{16}$O(n, α)$^{13}$C cross-section using a Double Frisch Grid Ionization ChamberNuclear Physics - TheoryNuclear Physics - ExperimentThe $^{16}$O(n, α)$^{13}$C reaction was proposed to be measured at the neutron time-of-flight (n_TOF) facility of CERN. To this purpose, a Double Frisch Grid Ionization Chamber (DFGIC) containing the oxygen atoms as a component in the counting gas coupled with a switch device in order to prevent the charge collection from the so-called γ-flash has been developed at Helmholtz-Zentrum Dresden-Rossendorf (HZDR), in Germany. The first $^{16}$O(n, α)$^{13}$C measurement without seeing the charge of the γ-flash at n_TOF has been performed in November 2018. After the electronics did not suffer from the γ-flash any more, another huge charge collection was discovered. Due to the high instantaneous flux at the n_TOF facility [1] the amount of that induced charge from neutron induced background reactions was piling up so much that the recognition of $^{16}$O(n, α)$^{13}$C reactions from that background was very difficult. For that reason another $^{16}$O(n, α)$^{13}$C measurement at the time-of-flight facility nELBE at HZDR which has a low instantaneous flux [2], has been performed in April 2019. Both measurements from n_TOF and nELBE will be presented here.oai:cds.cern.ch:28003642020
spellingShingle Nuclear Physics - Theory
Nuclear Physics - Experiment
Urlass, Sebastian
Beyer, Roland
Hammer, Sebastian
Hartmann, Andreas
Junghans, Arnd R
Kögler, Toni
Lutz, Benjamin
Mingrone, Federica
Müller, Stefan
Römer, Katja
Scheibler, Daniela
Stach, Daniel
Szücs, Tamás
Tassan, Laurent-Got
Turkat, Steffen
Wagner, Andreas
Weinberger, David
Measurement of the $^{16}$O(n, α)$^{13}$C cross-section using a Double Frisch Grid Ionization Chamber
title Measurement of the $^{16}$O(n, α)$^{13}$C cross-section using a Double Frisch Grid Ionization Chamber
title_full Measurement of the $^{16}$O(n, α)$^{13}$C cross-section using a Double Frisch Grid Ionization Chamber
title_fullStr Measurement of the $^{16}$O(n, α)$^{13}$C cross-section using a Double Frisch Grid Ionization Chamber
title_full_unstemmed Measurement of the $^{16}$O(n, α)$^{13}$C cross-section using a Double Frisch Grid Ionization Chamber
title_short Measurement of the $^{16}$O(n, α)$^{13}$C cross-section using a Double Frisch Grid Ionization Chamber
title_sort measurement of the $^{16}$o(n, α)$^{13}$c cross-section using a double frisch grid ionization chamber
topic Nuclear Physics - Theory
Nuclear Physics - Experiment
url https://dx.doi.org/10.1051/epjconf/202023901030
http://cds.cern.ch/record/2800364
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